Evaluation of the Small-animal Nano Scan PET/CT System using 89Zr

Author:

Alzimami Khalid1ORCID,Alanazi Sitah2,Gannam Magdi3,Alanazi Ahmad1ORCID,Aljamaz Ibrahim4,Alyanbawi Suliman4,Alotaibi Basem4,Almalki Yousif4ORCID,Sulieman Abdelmoneim5ORCID,Sassi Salem6

Affiliation:

1. Department of Radiological Sciences, College of Applied Sciences, King Saud University P. O.Box 10219, Riyadh 11433, Saudi Arabia

2. Department of Physics, College of Science, Imam Muhammad Ibn Saud Islamic University, Riyadh 11461, Saudi Arabia

3. Department of Physics and Astronomy, King Saud University, Riyadh, Saudi Arabia

4. Department of Cyclotron and Radiopharmaceuticals, King Faisal Specialist Hospital and Research Centre, P.O. Box 3354, Riyadh 11211, Saudi Arabia

5. Department of Radiology and Medical Imaging, College of Applied Medical Sciences, Salman bin Abdulaziz University. P.O.Box 422, Alkharj 11943, Saudi Arabia

6. Department of Medical Physics, Prince Sultan Military Medical City, Riyadh, Saudi Arabia

Abstract

Introduction: The purpose of the present work was to evaluate the imaging characteristics of 89Zr-PET in comparison with those obtained using fluorine-18 Fluorodeoxyglucose (18FFDG) PET (a gold standard tracer in PET imaging) using a small-animal NanoScan PET/CT scanner. Methods: The system’s spatial resolution, sensitivity, uniformity, and image quality were measured on a Nano Scan small-animal PET/CT scanner according to the NEMA NU4-2008 protocols. For reconstruction images, we used 2D and 3D reconstruction algorithms. The reconstruction methods included filter back projection (FBP), the ordered subsets expectation maximization (OSEM) algorithm, and the 3D Tera-Tomo algorithm, which are developed for the NanoScan small-animal PET/CT scanner. Results: The results obtained showed a significant difference in the spatial resolution for 89Zr as compared to 22Na and 18F when using a 2D reconstruction algorithm. The spatial resolution values were much enhanced by using the 3D Tera-Tomo reconstruction for each isotope, the Full width at half maximum (FWHM) values was less than 1 for all isotopes at the center of the field of view (FOV). This difference in spatial resolution is dependent on the positron range, energy, and the reconstruction method. Conclusion: The long half-life of 89Zr makes it an ideal positron emitter for performing immuno- PET, which is matched with the biological half-life of intact mAbs.89Zr can also give several advantages over other long half-life positron emitters in relation to the overall imaging performance because of its relatively short positron range and simpler decay scheme. The values of 89Zr sensitivity that were obtained in the present study were less than those of previous studies.

Funder

Strategic Technologies Program for National Plan for Science, Technology, and Innovation

Publisher

Bentham Science Publishers Ltd.

Subject

Radiology, Nuclear Medicine and imaging

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